US2447098A

US2447098A - Signaling system

Info

Publication number: US2447098A
Application number: US492491A
Authority: US
Inventors: Silverman Daniel
Original assignee: Stanolind Oil and Gas Co
Current assignee: Stanolind Oil and Gas Co
Priority date: 1943-06-28
Filing date: 1943-06-28
Publication date: 1948-08-17
Anticipated expiration: 1965-08-17

Description

ug. i?, 1948. D. slLvERMAN 2,447,098

SIGNALING SYSTEM Filed June 28, 1943 f 4 Sheets-Sheet l Eifer' Aug. l?, 194s. D. SILVRMAN 2,447,098

SIGNALING SYSTEM Filed June 28, 1945 4 Sheets-Sheet 2 ug 17 1948- D. SILVERMAN 2,447,098

SIGNALING SYSTEM Filed June 28, 1945 4 Sheets-Sheet 3 ugf 37, i948. D. slLvERMAN 2,447,098

S IGNALING SYSTEM Filed June 28, 1945 4 Sheets-Sheet 4 Patentecl ug. 17, 1948 SIGNALING SYSTEM Daniel Silverman, Tulsa, Okla., assignor to Stanolind Oil and Gas Company, |Tulsa, Okla., a corporation of Delaware Application une 28, 1943, Serial No. 492,491

1 Claim. 1

This invention pertains broadly to the art of electric signalling and has particular application in the eld of telemetering including well logging.

In many types of signalling systems such as the ordinary communication systems now in use, the eiect of the transmission medium is of relatively little importance. If there is large attenuation the amplitude can be increased at convenient points or a more sensitive receiver can be employed. However, in certain types of signalling systems the transmission medium is subject to large and variable attenuations. Accordingly in such systems it is nearly impossible to secure satisfactory quantitative results, particularly when employing telemetering. By telemetering is meant the measurement of a quantity, translating this measurement into an electrical signal, and receiving at least a portion of this signal at some distant point for measurement. Obviously if there is a variable attenuation in the transmission medium it is diflicult to interpret the received signal in terms of the amplitude of the transmitted signal. I am aware that in such cases recourse has been made to a frequency modulation system in which the original measurement is translated into a variation in frequency of the transmitted signals, there being a direct relationship between this variation in frequency and the quantity being measured. In such cases the amplitude of the signal received is of no essential importance provided only that it is great enough to be detected. The quantity being measured is detected in terms of the change in frequency of the signal.

However, one practical limitation of a frequency modulated telemetering system lies in the fact that it is necessary to calibrate the oscillator used in the transmitter in order to determine how much of the observed change in frequency is due to the quantity being measured and how much is actually due to drift in the frequency of the oscillator due to change in the various quantities of the circuit elements or of the potentials applied to the oscillator. There is another limitation in frequency modulated telemetering systems in those applications in which electrical noise or interference occurs between the transmitter and receiver or in the receiver itself. The energy in these spurious electric signals is a function of the Width of the band of frequencies being received. If the signal is weak it is necessary to limit the band of width being received to as small a value as possible in order to get the highest Value of `signal to noise ratio. Unless a high signal to noise ratio is obtained, no measurement can be made at the receiver since it will respond to the noise rather than to the signal. However, in the frequency modulation type of system a band of frequencies of considerable Width is necessary in order to permit transmission of a considerable variation in the quantity being measured. This condition is contradictory to the requirement for high signal to noise ratio.

It is an object of this invention to provide a method and means by which the band Width at the receiver can be extremely narrow while still permitting a wide variation in frequency for the transmission of the metering signals. It is a particular object of this invention to provide a means of maintaining a rst alternating current electric signal at a predetermined constant difference in frequency from a second alternating current signal, the frequency of which varies. Another object of this invention is to provide such a system in which a visual indication is produced proportional to the frequency of the controlled electric signal. Still a further object of this invention is to provide means for sharply filtering the difference in frequency between a transmitted signal and a signal generated by a local oscillator and utilizing the output of the sharp filtered waves to control the frequency of the local oscillator. Further objects and advantages of this invention will be apparent from this specification.

In general this receiving system for frequency modulated waves, particularly those in which the transmitted frequency is varied in accordance with a measurement made at a distant point, involves the use of a very low frequency sharply tuned filter to discriminate against noise. This filter operates on the output of a modulator or heterodyne detector that mixes the received signal plus noise and the output of a variable frequency oscillator. The output of this low frequency filter controls means for changing the frequency of the variable frequency oscillator in accordance with the amplitude of the output of the filter, in order to keep the frequency of the modulated signals fed into the lter constant in frequency. By this means the variable frequency oscillator produces a signal which is maintained at a constant difference in frequency from the transmitted frequency, this difference being the frequency of the filter.

In order to describe this invention in greater particularity certain figures have been attached hereto and are to be read in conjunction with this specification. In these figures the same reference numeral in different figures refers to the same or a corresponding part.

Figure 1 represents in block diagram form the Various elements used in generating and receiving the signals in one embodiment of my 1nvention; l i l Figure 2 is'a schematic diagram of apparatus used at a point of reception for the frequency modulated waves to carry out the functions shown in Figure 1;

Figure 3 is a representation 1n block diagram form of an alternative embodiment of my invention;

Figure 4 is a schematic diagram of apparatus used in conjunction with that of Figure 2 to carry out the alternative embodimentof my invention; Figure 5 represents invblock diagram form a third embodiment of the`invention;

Figure 6 is a graph of signal-frequency relationships; vr

Figures '7 and 8 are schematic diagrams or ap paratus for performing the functions set out 1n Figure '5.

Referring now to Figure 1, a measuring apparatu's II` which can be any of the systems already known in the art for producing an electric signal'in proportion to a quantity being measured, is connected to a frequency modulated oscillator I2, the frequency of which is controlled by the outputof this'measuring apparatus II. Preferably the output of this frequency modulated oscillator is amplied, for example by an amplifier i3, the output of which is impressed upon a transmission medium or transmitting line I4. Electrical disturbances or noise are impressed on this transmission medium. Such electric noise may involve the well known phenomenon identified as static or it may involve ground currents in the case'of well logging, etc. In all events a portion ofthe transmitted signal is received at a receiver along with'a certain quantity of this electrical noise. The input to the receiver is amplified by anI amplifier I5. This amplifier may and preferably does include a resonant circuit or a filter which' is broadly tuned to the range of frequencies to be'expected from the frequency modulated oscillator I2 and which thereby serves4 to attenuate electrical noise lying outside of this range of frequencies. However, this filter does not remove the'main disturbing elements in the noise spec# trum,v i. e., those lying within the range of frequency ofthe oscillator I2'.Y The output of amplifier I5I is maintained at substantially constant amplitude by a volume control means which may,

for example, be a limiter or an automatic volumev control system I6. The relatively constant output from` amplifier I5 is impressedon a modulator or" heterodyne detector I'I.` A variable frequency oscillator I8 is 'included in the receiver. The output of this oscillator is brought to a relatively constant amplitude, for example by passing it through an amplifier I9 which is controlled by an amplitude limiter or automatic volume control system 20; It is apparent that the transmitted signals plus noise are mixed with the output of the variable frequency oscillator inthe modulator or heterodyne detector I'I. The output from this modulator I'I contains various waves'includingl an alternating current wave at the difference of frequency of the received signals andthe frequency of the variable oscillator I8. The output of this modulator or heterodyne detector I'I is sharply filtered at a predetermined constant low frequency by a band pass filter 2I. The output or maybe an indicator of the amount of varia` from the band pass filter varies in amplitude dei pending upon the difference frequency between the input waves as compared to the peak frequency for which this filter is tuned. If this difference frequency is exactly equal to the peak frequency, the output of 4,filter 2I will be a maximunr'and since th'e lteriis'sharply tuned, the amplitude of the filtered output will drop off rapidly and vary approximately linearly as the difference frequency diverges from the peak frequency of the lter. It is to be noted that the sharply tuned band pass filter rejects components at all frequencies which are not very close to the peak frequency so that the waves in the output of the modulator which are proportional to the difference in the frequency of the noise and the frequency of the variable oscillator are very highly attenuated.

The output of the band pass filter 2I actuates a servo-mechanism 22; As is well known, a ser'vomechanism is'a device which produces motion ln` response to an electric signal, the amount of the motion being dependent upon the amplitude'of the applied signal and there being one pointat I' which for a certain applied signal intensity` thereA is no motion at all. For example, see Design and rFest of a High Performance Servo Mechanism," by H. L. Hazen, Journal of the Franklin Institute,

Vol. 218, pp. 543-580, November, 1934. This servo# mechanism 22 is employed to control or adjust the frequency of the variable frequency oscillator I8 by varying an electric circuit element in the resonant circuit of the oscillator. Accordingly the frequency of the oscillator is maintained at such a point that the output of the band pass filter 2I remains substantially constant'. Whenever the frequencycf the transmitted signal varies, the difference frequency likewise Varies, the output from the band lter changes in amplitude and the servo-mechanism 22 immediately changes the frequency of oscillator I8 until this quency from that of the received signal. Since the" band pass lter is tuned to a low frequency which should be less than cycles per second and preferably below 20 cycles per second, vfor example 1 to l2 cycles per second, and may be an electromechanical system of high effective Q, it is apparent that if the variation in frequency of oscillator 'I2 is of several hundred or thousand cycles per second, in effectv the variable'frequency oscillator is synchronized to oscillate at a frequency very closeto that of the oscillator' I2 and that thereby the variation in frequency of oscilla@ tor I8 is directly related to the signals put out by the measuring apparatus II. A visual indication is made which is proportional to the variation in frequency of the signals from oscillator I8, for example by indicator or recorder 23. This indicator may, for example,l be a frequency meter tionof the electric circuitelement inthe resonant circuit of lter I8 caused by operation of servomechanisrn 22. Still other examples of methods q of coupling vthis indicator to the system' will be shown in the following figures.'

In Figure 2 is shown a schematic wiring diagram of one arrangement of apparatus for carrying out the functions indicated in Figure 1. The incoming signal plus noise is impressed across the terminals Y-Y of the primary of a transformer 24, the secondary of which is connected to the grid of a first amplifying tube 25. The output from this tube is impressed upon the primary of transformer 26 across which is connected a condenser a by means of which the plate cincuit of tube 25 is broadly resonant in the range of frequencies to be expected from the frequency modulated transmitter and which thereupon reduces to some extent the amplified noise in the receiver. The output from transformer 25 is again amplified by amplifier tube 21. Amplifier tubes 25 and 21 are supplied with plate potential from a source such as battery 28 and are supplied with filament power from a source (not shown) in a manner obvious to those acquainted with vacuum tubes. Suitable bias circuits are supplied for these tubes in the conventional manner. The output of the second amplifier is impressed on transformer 28a. The secondary of this transformer impresses the amplified signal upon the control grid of a pentagrid mixer tube 3B. A center tapped tertiary winding 3! impresses a signal proportional to the amplified output from vacuum tube 2l on a double diode rectifier tube 32 producing a rectified output, the amplitude of which is proportional to the amplitude of the signals on winding 3i, across a resistor 33. This voltage is filtered by condenser 34 and

resistors

35, 36 and 31 and is applied to the control grids of Vacuum tubes 25 and 2l through the secondaries of

transformers

24 and 26 to adjust the gain of these two amplifier stages. Winding 3l, rectifier 32 and the associated apparatus constitutes an automatic volume control system of a known type which operates to maintain the output from the two amplifier tubes at a substantial constant maximum amplitude.

The variable frequency oscillator I8 shown in Figure 2 is a simple Hartley oscillator with a resonant circuit consisting of inductance 38 and variable tuning condenser 39. This resonant circuit is coupled to the oscillator tube 40 through condensers 4I so that the output from the oscillator on transformer 42 is substantially a sine wave the frequency of which depends rupon the setting of condenser 39. The output from this oscillator is amplified by vacuum tube 43 which is energized by a source of potential such as battery 44. The amplified output of tube 43 appears across transformer d5. volume control employed to maintain a constant output from amplifier tubes 25 and 21 could be used to secure a constant output from vacuum tube 43, it is equally satisfactory to employ a limiter circuit including Vacuum tube 46. The cathode of this pentode is connected directly to ground and the control grid is connected to ground through the secondary of transformer 45 in series with a resistor 51. Thus grid current flows as soon as the signal is applied and produces a bias that increases with the magnitude of the applied signal. This action is emphasized by operating the plate and screen grid of this pentode at a relatively low potential which is obtained by the use of dropping resistors 48 and 49. The increased signal decreases the gain of the tube and so maintains a substantially constant output voltage for any signal in excess of a given minimum. The amplifier tube 43 insures that this given minimum is always exceeded. There is While exactly the same system of slightamplitude distortion which is not objectionable in this application. The output from this limiter stage appears across the secondary of transformer 50 as a substantially constant output signal the frequency of which depends upon the capacity of tuning condenser 39. This signal is applied to the third grid of the pentagrid mixer tube 30. The output from this Crnixer tube includes various Waves of which one wave is produced by the heterodyning of the signal frequency of the input signal from the oscillator I2 with that from the local oscillator I8. If the frequencies of these two signals are fairly close together this difference frequency will be a very low audio f frequency. In order to segregate this difference frequency from those due to the action of noise, the output from the mixer across resistor 5I is coupled by condensers 52 to a very low frequency band pass filter 53. The characteristics of this band pass filter are shown in Figure 6 in a solid line, in which it is seen that the amplitude of output for a constant amplitude input decreases sharply on each side of the peak frequency fo. I have found by the employment of a Verylow frequency band pass filter, for example below 20 cy-cles`per second, I secure two distinct advantages in the operation of this system. In the first place, I can obtain extremely sharp filtering, i. e., the width of the pass band in cycles per second becomes only a few cycles. Second, since the output of this band pass filter is used to control the frequency of the variable oscillator I3, and in effect keep it almost in synchronism with the output of the oscillator I2, if fo is Very low there is very little difference between the frequencies of oscillator I2 and I8. Very low frequency sharply tuned filters suitable for this purpose may include multistage Scott circuits or more preferably an electro-mechanical filter cincuit such, for example, as described in Figure '7. As described therein, one such filter was constructed at a frequency of approximatelylZ cycles per second which had a pass band of approximately one cycle per second. Obviously using such a filter, the output of the filter 53 will sharply discriminate or attenuate that output of the mixer tube 30 which varies with the electrical noise.

In order to utilize the sharp filtering characteristics of the filter 53 properly, it is desirable to employ it to control the servo-mechanism about to be described. One satisfactory method of accomplishing this involves rectifying the output of the filter, for example by a full wave rectifier 54, the rectified output of which is applied to the coils of two relays 55 and 56. In order to secure a visual indication of the output of the filter, I prefer to include an indicating meter 5'! in this circuit. Relays 55 and 56 are adjusted so that under normal operating conditions the armature of relay 55 is closed against the action of a spring while the armature of relay 56 is held open by the action of another spring. An increase in output of the filter secured when the difference frequency applied to the input of this filter comes closer to the resonant frequency fo, closes relay 55 whereas swinging the difference frequency away from fo will result in the release not only of relay 56 but also of relay 55. When relay 55 closes it closes a circuit through a field winding 58 of a small series motor 59 through the armature and the source of power which is shown as battery B0. Switch 6I is, of course, closed at this time. The closing of this relay thereupon rotates the direct current motor which is connected through .frequency of oscillator I8.

18. amplified by amplifier 1I and impressed onfthe transmission medium or transmission line 12.

-gear train B2 to rotate a shaft 63 which injturn varies the setting of variable condenser. 39. This variation changes the frequency of oscillator I8 which changes the difference frequency applied to theV band pass filter 53 in such a sense as to increase the difference frequency, thus decreasing the output of the rectifier 54 and causing relay VSI5 to open, thus shutting off motor 59.

If this difference frequency becomes greater than normal, the output from band pass lter 53 decreases, thus causing the armature of relay 55 to open, closing the switch contacts of this relay through the second winding 64 of motor 59. This Winding is wound in opposition tothe field coil .58 and thus causes the .motor to rotate in the reverse direction, again adjusting condenser 39 which in turn adjusts the difference frequency from the mixer tube 38 to the value at which relay 55 again closes.

The position of shaft 63 is indicative of the Accordingly, a visual indication proportional to the relative motion of this shaft indicates the variation in frequency of oscillator I8 and in turn indicates the variation in frequency of the transmitting oscillator I2. A stylus 65 is mounted to rotate .with a gear of gear train 62 and is pressed against a strip of paper or similar material Et which is rolled onto a drum 61, for example by an electric motor 63. Thus the motion of the stylus on the paper produces a record directly related to the variation in frequency of oscillator I8. The paper strip or chart -66 may be moved longitudinally with respect to the stylus in any desired fashion. For example, in well logging this strip would be nor- -mally moved in direct relationship to the loweringl of the measuring apparatus II into the well in a manner which has been previously described in the art. If,y on the other hand, alvariation of frequency as a function of time is desired, the leads to motor-68 can be connected to any constant frequency source by means of which strip 66 will be moved at a substantially constant speed.

In case of necessity itis possible to eliminate the servo-mechanism. Thus, for example, by opening switch 6I the motor 59 is deenergized. Shaft-53 is provided with a hand wheel 69 which can be manually operated to vary the capacity 0f condenser 39. In this case the operator watches the meter. needle on meter 51, keeping it at a constant amplitude.

It is apparent that the synchronizing features of the invention have wide application in telemetering. In case a transmitter is used which is operated at a fairly constant frequencyI with a variable amplitude, thisginvention can still be employed, as shown in` Figure 3. Here the measuring apparatus I I operates to modulate the amplitude of an oscillator and amplitude modulator The output of this equipmentis preferably As before, it is assumed that this signal is attenuated as it passesthrough the mediumand that electrical noise is impressed thereon. A part of the received signallis passed through an amplifier and volume control 18 which produces a signal of substantially constant maximum output. This is impressed on the modulator I1, as is the signal from variable frequencyoscillator I8 Vwhich has similarly been passed through an amplifier and volume control apparatus`14. The output from the modulator is sharply Vfiltered bya low frequency band pass filter'2 I the amplitude of which .is utilized to actuate la servo-mechanism `22 which adjusts the frequency of the variable frequency oscillator I 8. Another portion of the input signal is amplified by amplier 15. In order to obtain an indication of the amplitude of the modulated signal it is necessary to demodulate the amplified output from amplifier 15, which can be accomplished satisfactorily by impressing this signal on a heterodyne detector or modulator 16 which is likewise fed with signals from the variable frequency oscillator I8. It is apparent that using this oscillator which Ahas been kept at a constant difference frequency from the frequency of oscillator 10 by the servo-mechanism 22, the output from modulator 'I6 will be at a constant difference frequency between the frequency of the signals of amplifier 15 and those from oscillator I 8 and that the amplitude of these output signals will vary with the amplitude of the signals from amplifier 15. A sharply tuned band-pass filter 11 similar to filter 2| is provided as the detector of the output from the modulator. The signals from this filter actuate the indicator 18 which produces a visual indication of the amplitude of the demodulated Wave. In this case the invention has been utilized to produce perfect tracking between the oscillator 18 and the local oscillator I8. It is to 'be understood that such a system would not be necessary if there is an accurate frequency control on oscillator 19. However, in telemetering applications in Well logging or logging-whiledrilling operations, such control is inherently infeasible and therefore serious errors would occur if no means were available to keep the local oscillator I8 operating at a constant difference frequency from that of oscillator 1U.

Figure 4 illustrates the 'additional equipment necessary to carry out the functions illustrated in Figure 3. The apparatus in Figure 2 is employed as before. Across Ypoints Y-Y in Figure 2 is connected the input to transformer 19, the secondary of which feeds the amplifier tube 80. The output of this stage is impressed through a resistance capacity coupling on the control grid of pentagrid mixer tube 8|. On the third grid of this mixer tube is applied the constant amplitude alternating current signal from point X on Figure 2 which is at the output of the transformer 50. The output from the pentagrid mixer tube 8l therefore contains a component at the difference 0f thelfrequencies between the amplitude modulated signal impressed on terminals Y-Y and the frequency of the signal at point X, with'an amplitude which varies in accordance with the modulation of the signal across the input to the receiver. This output across resistor 82 is ltered, preferably by a low frequency bandpass lter 83 and passed to the indicator shown generally by numeral 18. This can, for example, be made up of a full Wave rectifier 84, the output of which is filtered by the low frequency filter 84a and impressed on an oscillograph element 85,

, which therefore oscillates in relation to the de- .applied to a modulator or heterodyne detector I 1,

to which is valso applied the signal from the variable frequency oscillator I8. The output of the Vmodulator or heterodyne detector I1 is applied to a first lowfrequency sharply tuned band pass filter 88. The output of this filter is passed through an amplitude control 89 which brings the amplitude to a constant maximum value regardless of the frequency. The output of this amplitude oontrol is applied to a second sharply tuned low frequency band-pass filter 98. The output of this second filter is utilized to operate a frequency control mechanism 9| which may be a. servomechanism or may be any other type of electrical frequency control apparatus which adjusts the frequency of the variable frequency oscillator |8. The Variations in frequency of oscillator i8 are applied to a recorder 92 which produces a Visual indication varying in accordance with the frequency of oscillator i8. Preferably but not necessarily, `an indicator 93 is connected to the output of the second band pass filter 98 in order to indicate the Variation in output of this filter.

The operation of this embodiment of the invention can be considered to involve the following operations. The rst band pass filter 88 sharply discriminates against all signals except those at the difference -frequency corresponding to the pass band of filter 88, thus eliminating substantially all noise components. this signal is not constant since no amplitude control was employed on either of the signals applied to the modulator. However, the signal amplitude control 89 brings the output from the first band pass filter to a constant level. The second band pass filter 98 is tuned to a slightly different frequency from that of the first filter. The response of this filter may, for example, be shown by the dasl'ied line in Figure 6. It is apparent, therefore, that as the constant amplitude signal from f the amplitude control 89 passes through this second band pass filter that the amplitude of the output is going to vary depending upon the frequency. Any variation of this amplitude from a predetermined Value actuates the frequency con- .5

' determined by the first band pass filter 88. It

trol 9| to change the frequency of oscillator |8 in such a sense that the output of the second band pass filter 98 tends to be maintained at a constant level. By this means the frequency of oscillator |8 is maintained at a substantially constant r predetermined 4difference from that of the frequency modulated input from the transmission medium. 'I'his system has the advantage over that shown in Figure 1 in that only one amplitude control need be employed.

Apparatus suitable for carrying out the functions shown in Figure are found in the diagram of Figure '1. Here the input from the transmission medium is applied to transformer 94 by means of which it is applied to the first grid of the pentagrid mixer tube 95. The output from the variable frequency oscillator i8 is applied through transformer 42 to an amplifier tube 43. The output of this amplifier is applied through transformer 45 to the third grid of the mixer tube 95. The output of the mixer tube which with its circuits comprises the heterodyne detector or modulator |1, is applied to a first low frequency sharply tuned band pass filter 88 which, as shown, is of the electro-mechanical type. This consists of two

coils

96 and 91 which are insulated from but rigidly mounted on a mass 98 elastically suspended by suspension 99 from a case |88. Each of these coils is separately mounted to cut the flux of a magnetic field (not shown). The output of the heterodyne detector or modulator |1 drives the mass 98 by means of coil 96 at a frequency determined by the resonance of the mass and elastic suspension. This in turn vibrates coil 91 in its magnetic field generating voltage in, pro- The amplitude of i portion to its motion. By this means a very sharp low frequency band pass filter can be obtained. The output from this second coil 91 is amplified through a triode section of triode-pentode tube |8|. The signal on the plate of the triode section of this tube is coupled by condenser |82 to the control grid of the pentode section of the tube which is connected to the cathode through a resistor-condenser combination |83. This resistor is a grid leak which operates to keep th`e output volume from the pentode section of this tube substantially constant in exactly the same manner discussed in connection with the operation of vacuum tube 46 in Figure 2. The output from the pentode plate is coupled through a transformer |84 to a second low frequency sharply tuned band pass filter 98 which may, for example, be of the same type as that shown for the first band pass filter 88. As previously discussed, the tuned frequency of this filter is slightly different from that of the first band pass filter 88. Since the voltage applied through transformer |84 is of substantially constant amplitude, the Variation invthe output from this filter 98 varies only in accordance with the frequency. The output of this filter is applied to a servo-mech'anism which may, for example, be exactly the same as that shown in connection with Figure 2 including a rectifier 54, two relays 55 and 56 and an indicator 93. The two relays actuate the driving motor 59 .by means of battery 68, switch 6| and field coils 58 and 64. This motor drives shaft 63 through la gear train 62 and simultaneously drives a stylus 65 which is recording on a strip or chart 66 rolled on a drum 61 by an electric motor 68. The motion of shaft 63 rotates the variable plates of condenser 39, thus changing the frequency of oscillator I8 andadjusting this frequency until the difference frequency between the input signal and those from oscillator I8 are at the predetermined difference should be added that filter 98 is adjusted so that its peak frequency is sufficiently different from that of the first band pass filter 88 so that the variation in amplitude of the output is approximately linear in the neighborhood of the frequency fo. A second variant of the apparatus shown in block diagram form in Figure 5 is illustrated by Figure 8. The input signal from the frequency modulated source appears across the input transformer 94 and is impressed upon the control grid of the pentagrid mixer tube 95. As discussed below the third grid of this tube is actuated from the variable frequency oscillator so that the electron stream in the tube is rst modified by the received signal and then further varied by the oscillator potential. The signal output from this tube which includes an alternating current component at the difference in 4frequency of these two waves is applied across the primary of transformer which is preferably shunted by a condenser |86 which bypasses high frequency components of the output of the modulated signal. The output from transformer |85 is sharply filtered at a low frequency by band pass iilter88 which produces an output across transformer |86. The output from this transformer is brought to a uniform level, for example, by the amplitude control 89 which in this embodiment of the invention is shown as a limiter tube |81 with a grounded cathode and a grid circuit containing a grid leak |89. The tube is operated with low plate and screen grid voltages which in combination with the grid leak produces a bias which varies directly with the strength of the input signals, thus giving an output of substantially constant magnitude. Two or more of such limiters may be used in cascade if the amplitude is to be held to .extremely close limits. The output from this limiter is impressed on a sharply tunedfrequency discriminator which acts in the same fashion as does the band pass filter 99 shown in Figure 5, i. e., the output from this discriminator Varies approximately linearly with the variation in frequency of the constant amplitude signals in the amplitude control 89. The signals from the limiter are applied to transformer |09, the secondary of which is tuned by condenser to the desired low frequency. The signal is likewise capacitively coupled by condenser III and resistor` I|2 to the center tap on the secondary of the tuned transformer. The resultant signal on each half of Vthe circuit is applied through a diode rectier ||3 across a resistor I |4 across which are shunted bypass condensers ||5. Brieiiy when the frequency of the constant amplitude signals applied vto transformer |09 is at the desired frequency difference to which' the secondary is tuned, no signal appears between the cathodes of the two tubes, but when the frequency varies from this value a D. C. voltage does appear, the magnitude of which varies with the divergence of the applied frequency from the tuned frequency. For a more .complete description of this phenomenon reference is made to Fundamentals of Vacuum Tubes, by A. V. Eastman, second edition, McGraw-lill Book Company, 1941,.,pages 537 to 540. The variation in voltage between cathodes of the diodes I I3 is read on the indicator 93 which is preferably a vacuum tube voltmeter of conventional design with high input resistance. This varying signal is likewise applied to the control grid of a so-called reactance tube ||6 .which is connected in the resonant ycircuit of the vacuum tube oscillator I8.

The Icathode of vacuum tube I|6 is ellectively connected to the lower point of the inductance II'l which with condenser ||8 forms a resonant circuit for oscillator tube I I9. The plate is directly coupled to the other end of this inductance. The signal across this inductance is applied across a phase shifting network made up of resistor and condenser IZI, and the Voltage across the resistor is applied to the control grid of Vtube I I6. Since this grid effectively controls the amount of plate current regardless of the variation in plate potential, it follows that since this grid potential is approximately 90 out of phase with the plate potential that the plate current will be similarly 90 out of phase with th'e plate current so that the Vacuum tube II 6 will act as a reactance shunted across inductance II'I. The value of this reactance is governed by the gain of the tube, which is determined by the bias between control grid and cathode of this tube. This bias is governed by th'e Voltage between the cathodes of the discriminator of the diodes II3. Hence whenever the frequency applied to transformer |09 deviates from the value at which there is Zero voltage between cathodes of diode I I3 the eiective reactance of the reactance tube IIB is altered, thereby changing the frequency of the oscillator tube II9.V Th'e frequency of this oscillator is varied in such a direction as to correct `for the variation indifference frequency applied to transformer |09. The output from the oscillator ||9 is preferably but not necessarily adjusted to a constant amplitude by passing the signal through a limiter tube |22 which has a grounded cathode and a grid leak resistor I 23. The plate and screen CTI grid of this tube are operated at a low potential through dropping resistor |24. Tll'e limited output from this stage is applied through transformer |25 to the third grid of the mixer tube to lcomplete the .control action.

A recorder 92 which is preferably an electron tube type frequency meter of any of theV well known types is connected :across the secondary of the transformer |25. It thereby indicates th'e frequency from oscillator I8 which by the control system described herein is maintained at `a predetermined constant difference in frequency from the input alternating current signal applied to transformer 94.

It is apparent that the invention described herein is capable of Wide application and that the various embodiments which have been sh'own and `described are but specific examples of which many others will be apparent to those skilled in the art. There is no intention of limiting the invention to the apparatus described; it is best set forth in the appended claim.

Iclaim:

In a system for demodulating frequency-modulated signals received in the presence of a very large noise background, th'e frequency of said signals being varied slowly in accordance with slowly changing transmitted intelligence, the combination comprising: receiving means for said frequency-modulated signals together with said noise, an oscillator containing at least one adjustable reactance and adapted to generate alternating potentials over approximately the same frequency range as the received signals, a modulator connected to said receiving means and to said oscillator, a first sharply tuned band-pass filter connected across the output of said modulator, said lter being tuned to frequency not greater than cycles per second, means for maintaining the output of said lter at an approximately constant average amplitude, a second sharply tuned band-pass lter directly connected to the output of said amplitude-maintaining means and tuned to a frequency differing from but within the pass band of said rst lter, and a servo-mechanism controlled lonly by the amplitude of the output of said second filter and adapted to vary the value of said adjustablereacta-nce as the average amplitude of said second lter output varies from a fixed predetermined value, whereby said second lter output is maintained approximately const-ant and the frequency of said oscillator is maintained at a constant frequency difference from that of said signals.

DANIEL SILVERMAN.

REFERENCES CITED The following references are of record in the file of this patent:

UNITED STATES PATENTS Number Name Date 1,999,215 Smith Apr. 30, 1935 2,041,855 Ohl Mar. 26, 1936 2,112,826 Cook Apr, 5, 1938 2,121,103 Seeley June 2l, 1938 2,126,910 Moselly Aug. 16, 1938 2,165,510 Rosene July 11, 1939 2,192,022 Wills Feb. 27, 1940 2,233,198 Dome Feb. 25, 1941 2,245,685 Koch June 17, 1941 2,379,689 Crosby July 3, 1945 2,380,947 Crosby Aug. 7, 1945 2,396,360 Ziegler Mar. 12, 1946